1979
DOI: 10.1107/s0021889879013042
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A double focusing X-ray camera for use with synchrotron radiation

Abstract: A double focusing camera for synchrotron radiation is described. Focusing in the vertical plane is achieved with a segmented mirror whereas in the horizontal plane a bent triangular monochromator is used. The entire system is remotely controlled. A few examples of results obtained on biological samples illustrate the performance of the instrument.

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Cited by 131 publications
(36 citation statements)
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“…It does not touch the primary beam and therefore does not need to be included in the beamline analysis. Apart from the relative positions of mirror and monochromator, the present set-up is equivalent to those described by Yoda (1984), Furuno, Sasabe & Ikegami (1987), Hayashi, Hamada, Suehiro, Masaki, Ogawa & Miyaji, (1988) and Riekel & Suortti (1991) for rotating-anode sources and those described by Barrington Leigh & Rosenbaum (1974), Webb, Samson, Stroud, Gamble & Baldeschwiler (1977), Hendrix, Koch & Bordas (1979) and Amemiya, Wakabayashi, Hamanaka, Wakabayashi, Matsushita & Hashizume (1983) for synchrotron-radiation sources. We have chosen this set-up as it is the most common, even though it employs a perfect-crystal monochromator and that the resolution function due to this has a very small contribution from the wavelength spread.…”
Section: Examplementioning
confidence: 99%
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“…It does not touch the primary beam and therefore does not need to be included in the beamline analysis. Apart from the relative positions of mirror and monochromator, the present set-up is equivalent to those described by Yoda (1984), Furuno, Sasabe & Ikegami (1987), Hayashi, Hamada, Suehiro, Masaki, Ogawa & Miyaji, (1988) and Riekel & Suortti (1991) for rotating-anode sources and those described by Barrington Leigh & Rosenbaum (1974), Webb, Samson, Stroud, Gamble & Baldeschwiler (1977), Hendrix, Koch & Bordas (1979) and Amemiya, Wakabayashi, Hamanaka, Wakabayashi, Matsushita & Hashizume (1983) for synchrotron-radiation sources. We have chosen this set-up as it is the most common, even though it employs a perfect-crystal monochromator and that the resolution function due to this has a very small contribution from the wavelength spread.…”
Section: Examplementioning
confidence: 99%
“…The numerical example calculated in the following is based on the set-up described by Hendrix et al (1979) using the storage ring DORIS at DESY in Hamburg as radiation source. For the flux measurements performed by Hendrix et al, the ring was • l rad -2 mm-2 operated at 4-7 GeV at a current of 20 mA.…”
Section: -(Z3mentioning
confidence: 99%
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“…Mirrors present severe technological problems because the small angles of incidence mean that they must be long, of the order of a few metres, and even segmented mirrors are difficult to support and align. Double focusing has been achieved on the storage ring DORIS (Hamburg, Federal Republic of Germany), where a photon flux of 5___ 2 x 10 xx photons s-1 in a focal spot of 1.1 mm diameter was measured (Hendrix, Koch & Bordas, 1979), but the focal region was surrounded by a high background area of 200 mm 2, caused by stray radiation scattered from the various components placed in the optical path. A toroidal mirror and double germanium crystal monochromator have been used at SPEAR (Stanford, USA) by Hastings, Kincaid & Eisenberger (1978) to produce double focusing; however, economic considerations may prevent further use of toroidal mirrors because of the difficulties in manufacture.…”
Section: Discussionmentioning
confidence: 99%
“…3). This principle has since been incorporated with a different mechanical design in monochromators used at EMBL, Hamburg (Hendrix, Koch & Bordas, 1979) and at SRS, Daresbury (Helliwell & Worgan, 1979). The whole optical path is under vacuum.…”
Section: Monochromatormentioning
confidence: 99%